NZ248122A - Compensating for chromatic dispersion of wavelength division multiplexed optical signals - Google Patents
Compensating for chromatic dispersion of wavelength division multiplexed optical signalsInfo
- Publication number
- NZ248122A NZ248122A NZ248122A NZ24812293A NZ248122A NZ 248122 A NZ248122 A NZ 248122A NZ 248122 A NZ248122 A NZ 248122A NZ 24812293 A NZ24812293 A NZ 24812293A NZ 248122 A NZ248122 A NZ 248122A
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- NZ
- New Zealand
- Prior art keywords
- optical
- dispersion
- compensating
- optical signals
- multiplexed
- Prior art date
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Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29379—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means characterised by the function or use of the complete device
- G02B6/29392—Controlling dispersion
- G02B6/29394—Compensating wavelength dispersion
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/25—Arrangements specific to fibre transmission
- H04B10/2507—Arrangements specific to fibre transmission for the reduction or elimination of distortion or dispersion
- H04B10/2513—Arrangements specific to fibre transmission for the reduction or elimination of distortion or dispersion due to chromatic dispersion
- H04B10/2525—Arrangements specific to fibre transmission for the reduction or elimination of distortion or dispersion due to chromatic dispersion using dispersion-compensating fibres
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04J—MULTIPLEX COMMUNICATION
- H04J14/00—Optical multiplex systems
- H04J14/02—Wavelength-division multiplex systems
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B2210/00—Indexing scheme relating to optical transmission systems
- H04B2210/25—Distortion or dispersion compensation
- H04B2210/252—Distortion or dispersion compensation after the transmission line, i.e. post-compensation
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B2210/00—Indexing scheme relating to optical transmission systems
- H04B2210/25—Distortion or dispersion compensation
- H04B2210/254—Distortion or dispersion compensation before the transmission line, i.e. pre-compensation
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- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Chemical & Material Sciences (AREA)
- Dispersion Chemistry (AREA)
- Electromagnetism (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Communication System (AREA)
Description
<div class="application article clearfix" id="description">
<p class="printTableText" lang="en">Priority Date(s): 1.7?. 1.. <br><br>
Complete Specification Filed: ...!3.).?.l9.3>. <br><br>
Class: (6) <br><br>
„/..i.55. <br><br>
: Publication Date: <br><br>
i i P.O. Journal No: <br><br>
2 6 MAR 1996 <br><br>
IH-o-2. <br><br>
24 8 1 22 <br><br>
ORIGINAL <br><br>
NEW ZEALAND PATENTS ACT 1953 COMPLETE SPECIFICATION <br><br>
I 12JUL 19 93 <br><br>
"MULTIPLE WAVELENGTH DIVISION MULTIPLEXING SIGNAL <br><br>
COMPENSATION" <br><br>
WE, ALCATEL AUSTRALIA LIMITED, 5oo OO <br><br>
A Company of the State of New South Wales, of 280 Botany Road, Alexandria, New South Wales, 2015, Australia, hereby declare the invention for which we pray that a patent may be granted to us, and the method by which it is to be performed, to be particularly described in and by the following statement: <br><br>
5 3 <br><br>
1 <br><br>
*48 122 <br><br>
This invention relates to electronics and more particularly to fiber optic communications systems. Even more particularly, the present invention relates to a method and system to increase the usable wavelength range of a wavelength division multiplexed optical path by achieving zero chromatic 5 dispersion near desired wavelengths of operation. <br><br>
In optical fibre networks, wavelength division multiplexing (WDM) uses a device known as a wavelength division multiplexer to multiplex individual optical signals into a single multiplexed signal that a single optical fibre can carry. WDM is generally used when the number of fibres in an existing transmission 10 link is inadequate or designing a system with a sufficient number of fibres becomes cost prohibitive. <br><br>
WDM systems often operate at frequencies other than the frequency for which an existing transmission link may best operate. For example, some WDM systems may operate at optical frequencies of between 1540 and 1550 nm, 15 while the existing transmission link may be designed to array a signal having a 1310 nm wavelength. For these instances, undesirable optical chromatic dispersion may occur in the optical path. The optical fibre path for a WDM system, therefore, may require chromatic dispersion compensation to achieve desired performance characteristics. <br><br>
20 Optical fibre compensation is usually selected to reduce the chromatic dispersion to zero at a wavelength near the planned wavelength of operation. This wavelength is called the dispersion-zero or zero-chromatic-dispersion wavelength. In some types of dispersion compensation, both positive and <br><br>
2 <br><br>
24 8 12? <br><br>
negative residual chromatic dispersion, may persist at wavelengths other than the dispersion-zero wavelength. This remaining chromatic dispersion may limit the usefulness of the optical fibre transmission path, because the non-zero dispersion may compromise or preclude transmission of optical signals having 5 frequencies other than the dispersion-zero frequency <br><br>
C. Lin, H. Kogelnik, and L. G. Cullen, "Optical-Pulse Equalization of Low-Dispersion Transmission in Single-Mode Fibres in the 1.3 - 1.7 //m Spectra Region," Optics Letters, v.5, No. 11 (Nov. 1980), describes an optical-pulse-equalization technique for minimizing pulse dispersion in a single-mode fibre 10 transmission system. The technique uses the positive and the negative dispersion characteristics of single-mode fibres on both sides of a dispersion-zero wavelength. While the technique is successful in controlling chromatic dispersion for a single wavelength, it does not address the problem of providng compensation over a band of wavelengths. <br><br>
15 It is therefore an object of the present invention to provide a method and system to simultaneously and independently control chromatic dispersion of independent optical signals that are to be wavelength division multiplexed for transmission. <br><br>
It is an object of the present invention to provide a system that permits 20 simultaneous and independent control of optical dispersion at any desired wavelength to increase the usable wavelength range of optical signals for wavelength division multiplexing. To achieve these results, the present invention individually compensates optical dispersion of all signals associated <br><br>
3 <br><br>
24 8 1 p ? <br><br>
with a wavelength division multiplexer. This is in addition to the dispersion compensation that the multiplexed signal itself experiences. The method and system undercompensates the multiplexed optical signal by a predetermined amount so that each of the optical signals has an associated residual optical 5 dispersion. To eliminate the residual optical dispersion, each of the optical signals is compensated individually to produce a zero optical dispersion along each individual optical path that will receive the demultiplexed optical signals. Consequently, each of the optical signals that make up the multiplexed optical signal has minimal chromatic dispersion upon receipt. <br><br>
10 It is also an object of the present invention to permit modular interchanging or replacement of different optical signal transmitters while maintaining the same performance along the wavelength division multiplexed signal path. By selecting individual compensation to match the precise wavelength of the individual transmitter and, then, including the individual 15 residual dispersion compensation as a modular part of the optical signal transmitter itself, the present invention permits non-disruptive interchanging or replacement of dispersion compensated transmitters. <br><br>
According to the invention there is provided a method for compensating optical chromatic dispersion of a plurality of optical signals associated with a 20 wavelength division multiplexer that forms a multiplexed optical signal from said plurality of optical signals, comprising the steps of undercompensating said multiplexed optical signal by a predetermined amount so that each of said optical signals has an associated residual optical dispersion; and compensating <br><br>
4 <br><br>
2 4 8 1 ? 9 <br><br>
individually each of said optical signal to remove therefrom said residual optica! dispersion. <br><br>
In order that the invention may be readily carried into effect, embodiments thereof will now be described in relation to the accompanying drawings, in 5 which: <br><br>
Figure 1 provides a plot of chromatic dispersion versus wavelength to illustrate the effects of compensating dispersion in a wavelength division multiplexed signal; <br><br>
Figure 2 provides a simplified block diagram of the preferred embodiment 10 of the present invention; and <br><br>
Figure 3 provides an alternative embodiment of the present invention. <br><br>
The preferred embodiment of the present invention is best understood by referring to the figures wherein like numerals are used for like and corresponding parts of the various drawings. <br><br>
15 The method and system of the preferred embodiment increase the useable wavelength range of a wavelength division multiplexed signal by essentially eliminating residual dispersion in the individual optical paths that form a wavelength division multiplexed signal. The present invention takes advantage of the fact that in WDM systems, the wavelength of each optical transmitter 20 feeding into a wavelength division multiplexer is known, as are the dispersion characteristics for frequencies above and below a predetermined dispersion-zero wavelength. With this information, it is possible to individually compensate the individual optical signals either prior to multiplexing or after demultiplexing the <br><br>
5 <br><br>
signal. For example, when compensating a standard 1310 nm optimized single-mode fibre ti operate in the 1 550 wavelength window, the fibre may be undercompensated as a whole. Then, either prior to multiplexing or after demultiplexing, additional compensation may be added for each wavelength 5 signal feeding into the WDM. The result is that each signal that the WDM system carries will be operating at a near zero dispersion level for its individual optical signal wavelength. <br><br>
Referring to Figure 1, there is shown a particular example of the effects of dispersion compensating a WDM output signal as well as the effects of this 10 dispersion at wavelengths other than the dispersion zero wavelength. Along the ordinate of the graph of Figure 1 is an abbreviated plot of chromatic dispersion in ps/nm ranging from -200 to 5600 ps/nm. Along the abscissa of Figure 1 appears an abbreviated range axis for optical signal wavelengths in nm ranging from zero to 1560 nm. Within the plot of Figure 1 appear three lines of 15 approximately equal slope for an exemplary 300 km fibre span of standard 1310 nm optimized fibre. <br><br>
Curve (a) of Figure 1 shows the uncompensated chromatic dispersion versus wavelength curve ranging from 5220 ps/nm at a wavelength of 1540 nm through a point of 5400 ps/nm at 1550 nm to a outer point, for example, of 20 5580 ps/nm at a 1560 nm wavelength. An equation for curve (a) may be stated as follows: <br><br>
Dispersion = 18- (wavelength - 1250 nm) [ps / nm) <br><br>
(1) <br><br>
Suppose further that in order to compensate for optical dispersion at the <br><br>
6 <br><br>
24 8 1 P <br><br>
« U- m wavelength of 1550 nm, a -5400 ps/nm dispersion compensator compensates the output of a WDM. In such an instance, 1550 nm is the dispersion zero wavelength. This causes the values of equation (1) to shift according to the following formula: <br><br>
than the 1550 nm dispersion-zero wavelength chromatic dispersion affects the optical signal. Chromatic dispersion is negative for wavelengths less than 1550, (e.g., -180 ps/nm chromatic dispersion at 1540 nm) and positive for wavelengths greater than 1550 nm (e.g., +180 ps/nm at a wavelength of 1560 10 nm). The residual dispersion that occurs at other than the dispersion-zero wavelength of the multiplexed signal, therefore, adversely affects and limits the use of an optical fibre path for carrying a WDM output signal. In fact, for those signals above and below the dispersion-zero wavelength, several important optical signals may be compromised or even fully precluded. 15 The method and system of the preferred embodiment overcome this problem by providing a combination of undercompensation that yields at least a smail positive amount of residual chromatic dispersion at the shortest wavelength that may travel along a standard fibre as a WDM output. For example, curve (c) of Figure 1 shows that at the lowest wavelength of the 20 example (i.e., 1540 nm) yet a small degree of undercompensation (i.e., 20 <br><br>
ps/nm) remains as residual chromatic dispersion when the previous dispersion-zero wavelength of 1550 nm is compensated only by -5200 ps/nm. From this <br><br>
Dispersion = 18- (wavelength - 1550 nm) \ps/nm\ <br><br>
(2) <br><br>
5 <br><br>
Curve (b) shows a plot of equation (2). Note that at wavelengths other <br><br>
2i ' <br><br>
point, chromatic dispersion will increase as the wavelength increases to, for example, a wavelength of <br><br>
1560 nm to reach a residual chromatic dispersion value of +380 ps/nm. The preferred embodiment provides not -5400 ps/nm as was used in 5 curve (b), but rather only -5200 ps/nm to yield a +200 ps/nm chromatic dispersion at the 1550 nm wavelength. With this degree of undercompensation, the preferred method and system then individually compensate for the residual dispersion associated with each of the wavelengths associated with WDM. <br><br>
10 illustrate the inventive concept. Referring to Figure 2, there is shown a WDM optical transmission system 10 that includes, for example, three optical transmitters such as XMT1 designated as 12 for transmitting a signal having a wavelength A equal to 1540 nm, XMT2 designated as 14 for transmitting a wavelength of 1550 nm, and XMT3 designated as 16 for transmitting a 15 wavelength of 1560 nm. Each of the optical signal transmitters feed to residual dispersion compensators. For example, dispersion comparator 18 receives output from XMT1 12, dispersion compensator 20 receives signals from XMT2 14, and dispersion compensator 22 receives optical signals from optical transmitter XMT3 16. Outputs from dispersion compensators 18, 20 and 22 go 20 to WDM 24. WDM 24 provides a single output signal that goes to dispersion compensator 26 for compensating the WDM 24 multiplexed signal. From the dispersion compensator 26, the multiplexed optical signal travels along, for example, 300 km standard fibre 28 that ultimately goes to wavelength division <br><br>
Figure 2 specifically shows the preferred embodiment to more fully <br><br>
8 <br><br>
2 4 S 1 p p hp* <br><br>
demultiplexer 30. After demultiplexing the optical signal it receives, wavelength division demultiplexer 30 transmits the individual optical signals to individual receivers designated as RCVR1 having reference numeral 32, RCVR2 designated by reference numeral 34 and RCVR3 designated by reference numeral 36. <br><br>
5 The system of Figure 2 takes into consideration the known operating characteristics of a system having a dispersion-zero wavelength of 1550 nm and a positive or increasing rate of chromatic dispersion versus wavelength. In the example of Figure 2, instead of providing a -5400 ps/nm dispersion compensator (as is the case of curve (b) of Figure 1), the method and system of the preferred 10 embodiment provide only a -5200 ps/nm dispersion compensator. The res*j!t is that at the dispersion-zero wavelength of 1550 nm, a residual dispersion of 200 ps/nm exists. Also, at the 1540 nm wavelength, a positive chromatic dispersion of ps/nm occurs of +20 ps/nm. This contrasts with the -180 ps/nm chromatic dispersion that would exist if a -5400 ps/nm dispersion compensator were used 15 as dispersion compensator 26 of Figure 2. Similarly, in curve (c) of Figure 1, <br><br>
instead of a +180 ps/nm chromatic dispersion at a 1560 nm wavelength, a + 380 ps/nm optical dispersion occurs. <br><br>
To compensate for these positive chromatic dispersion values existing when using only a -5200 ps/nm dispersion compensator 26, the preferred 20 embodiment uses the discrete residual chromatic dispersion compensators 18, 20 and 22 of Figure 2. In particular, dispersion compensator 18 provides -20 ps/nm of optical dispersion for the 1540 nm optical signal from XMT1 12. Dispersion compensator 20 provides -200 ps/nm of residual chromatic <br><br>
9 <br><br>
2.4 8 1 p o dispersion compensation for the optical signal from XMT2 14. Dispersion compensator 22 provides -380 ps/nm for the 1560 nm optical signal from XMT3 16. This preliminary chromatic dispersion compensation assures that all the signals reaching WDM 24 have a chromatic dispersion of +5200 ps/nm. Then, 5 at dispersion compensator 26, the multiplexed output from WDM 24 is compensated by an amount of -5200 ps/nm so that each of the signals comprising multiplexed signal output from WDM 24 operates at a near zero optical dispersion upon being transmitted along 300 km standard fibre 28. <br><br>
Then, at wavelength division demultiplexer 30, the compensated multiplexed 10 signal is then demultiplexed and sent to receivers RCVR1 32, RCVR2 34, and RCVR3 36. <br><br>
The method and system of the preferred embodiment have several important advantages. For example, by first undercompensating all of the optical signals from the optical transmitters, there exists the residual chromatic 15 dispersion that can be eliminated to produce uniform chromatic dispersion level. Additionally, by individually compensating residual chromatic dispersion in each optical path, the simultaneous and independent control of optical dispersion is possible for any desired wavelength. This permits matching compensation to an optical transmitter prior to installing the transmitter in a WDM system. In fact, 20 by permitting the selection of matching compensation prior to connecting an optical source to a WDM system, the preferred method and system permit packaging the residual dispersion compensation with a transmitter. This may be done during transmitter manufacture to ensure that residual dispersion <br><br>
10 <br><br>
24 8 | v compensation is as precise as possible. <br><br>
Figure 3 shows an alternative embodiment 40 of the present invention. In particular, optical transmitters XMT1 12, XMT2 14, and XMT3 16 all feed directly to WDM 24. Output from WDM 24 goes to -5200 ps/nm dispersion 5 compensator 26 and then to 300 km standard fibre 28. At the receiving end, the multiplexed signal from 300 km standard fibre 28 goes to wavelength division demultiplexer 30 for demultiplexing. Then, in contrast to the preferred embodiment, each of the demultiplexed optical signals go to respective dispersion compensators 18, 20 and 22. Dispersion compensator 18 provides -10 20 ps/nm dispersion compensation for the demultiplexed 1540 nm optical signal, dispersion compensator 20 provides <br><br>
-200 ps/nm compensation for the demultiplexed 1550 nm optical signal, and dispersion compensator 22 provides <br><br>
-380 ps/nm dispersion compensation for the demultiplexed 1560 nm optical 15 signal. Receiver RCVR1 32 receives the compensated output from dispersion compensator 18, RCVR2 34 receives the compensated output from dispersion compensator 20, and RCVR3 36 receives the compensated output from dispersion compensator 22. <br><br>
In essence, a distinction between the preferred embodiment of Figure 2 20 and the alternative embodiment of Figure 3 is that instead of compensating for local residual optical dispersion prior to wavelength division multiplexing at WDM 24, the alternative embodiment compensates for local residual dispersion at the output of wavelength division demultiplexer 30. In such an instance, for <br><br>
11 <br><br>
2 4 0 * <br><br>
o ) 9 p s £■-1, C, <br><br>
example, each receiver 32, 34 and 36 may include prepackaged residual dispersion compensators such as dispersion compensators 18, 20, 22, respectively, that may be installed during receiver manufacture. Finally, a combination of local residual dispersion compensation both before receipt of the 5 optical signal at WDM 24 and after demultiplexing at wavelength division demultiplexer 30 may be attractive for some applications. <br><br>
Although, given the above description of Figures 2 and 3, it may be intuitive how the preferred multiple WDM signal system compensation network 10 of the preferred embodiment operates to individually compensate for residual 10 dispersion, the following discussion describes the system as a whole by following an exemplary signal flow from transmission to receipt. For example, referring again to Figure 2, suppose that three signals, one having a wavelength of 1540 nm, another having a wavelength of 1550 nm, and yet a third of having a wavelength 1560 nm are to be transmitted along a 300 km standard 1310 nm 15 optimized fibre. <br><br>
To transmit these signals, XMT1 12 sends the 1540 nm signal to -20 ps/nm dispersion compensator 18, XMT2 14 sends the 1550 nm signal to -200 ps/nm dispersion compensator 20, and XMT3 16 sends the 1 560 nm signal to -380 ps/nm dispersion compensator 22. Each of these signals simultaneous and 20 independently go to WDM 24 where they are multiplexed into a single multiplexed WDM output signal. This WDM output signal is then sent directly to -5200 ps/nm dispersion compensator 26 which provides -5200 ps/nm of chromatic dispersion compensation. <br><br>
12 <br><br>
2 4 o i 9 9 <br><br>
augi <br><br>
The output of the -5200 ps/nm dispersion compensator 26 has approximately zero chromatic dispersion after it exits the 300 km standard 1310 nm optimized fibre 28. This multiplexed signal then goes to wavelength division demultiplexer 30, where it is demultiplexed into three signals having respective 5 wavelengths of 1540 nm, 1550 nm, and 1560 nm. Each of the optical signals have an approximately zero chromatic dispersion and go to associated receivers RCVR1 32, RCVR2 34 and RCVR3 36. <br><br>
The operation of the alternative multiple WDM signal compensation network 40 at Figure 3, again, is similar to that of Figure 2, except that local 10 residual chromatic dispersion compensation does not take place until after the signal is demultiplexed by wavelength division demultiplexer 30. <br><br>
In summary, the preferred method and system provide a multiple WDM signal compensation network that eliminates residual dispersion compensation and overcomes limitations associated with single dispersion compensation 15 networks by undercompensating the multiplexed optical signal by a predetermined amount so that each of the optical signals that feed into a WDM has an associated residual optical dispersion and, then, either before or after multiplexing takes place, compensating individually each of the optical signals to remove the residual optical dispersion. This avoids the problems that residual 20 chromatic dispersion can induce that may make certain signals in a WDM multiplexed signal unacceptable for high data rate operations. <br><br>
Although the invention has been described with reference to the above-specified embodiments, this description is not meant to be construed in a <br><br>
13 <br><br>
248199 <br><br>
* Cc. <br><br>
limiting sense. Various modifications of the disclosed embodiment, as well as alternative embodiments of the invention, will become apparent to persons skilled in the art upon reference to the above description. It is, therefore, contemplated that the appended claims will cover such modifications that fall within the true scope of the invention. <br><br></p>
</div>
Claims (11)
1. A method for compensating optical chromatic dispersion of a plurality of optical signals associated with a wavelength division multiplexer that forms a multiplexed optical signal from said plurality of optical signals, comprising the steps of:<br><br> compensating the chromatic dispersion of the multiplexed optical signals by a predetermined amount so that each of said optical signals has a residual optical dispersion; and compensating individually the chromatic dispersion of each of said optical signals to remove therefrom said residual optical dispersion.<br><br>
2. A method for increasing the usable wavelength range of an optical fibre path, comprising the steps of:<br><br> forming a multiplexed optical signal for transmission along said optical path from a plurality of optical signals,<br><br> compensating the chromatic dispersion of said multiplexed optical signal by a predetermined amount so that each of said optical signals has a positive residual optical dispersion when transmitted along said optical path; and compensating individually the chromatic dispersion of each of said optical signals to remove therefrom said residual optical dispersion to thereby permit transmission along said optical path with minimal optical dispersion for each of said optical signals.<br><br>
3. A method for discretely compensating a plurality of optical signals associated with a wavelength division multiplexer, comprising the steps of:<br><br> multiplexing a plurality of optical signals with a wavelength divtsjpn<br><br> 15<br><br> 24 8 1 2 2<br><br> multiplexer to form a multiplexed optical signal;<br><br> compensating the chromatic dispersion of said multiplexed optical signal by a predetermined amount so that each of said optical signals has a residual optical dispersion;<br><br> 5 compensating individually the chromatic dispersion of each of said optical signals by a predetermined discrete amount to remove therefrom said residual optical dispersion.<br><br>
4. A method for approximating a dispersion-zero wavelength in a plurality of optical paths, comprising the steps of:<br><br> 10 associating a wavelength division multiplexer with said plurality of optical paths each carrying an optical signal from an associated optical signal transmitter; generating a multiplexed optical signal from said wavelength division multiplexer;<br><br> compensating the chromatic dispersion of said multiplexed optical signal by a predetermined amount so that each of said optical signals has a residual optical 15 dispersion; and compensating individually the chromatic dispersion of each of said optical signals to remove therefrom said residual optical dispersion, thereby causing each of said optical signals to be transmitted at approximately a dispersion-zero wavelength for each of said optical paths.<br><br> 20
5. A method of matching dispersion compensation to an optical wavelength, comprising the steps of:<br><br> generating said plurality of optical signals to each have a predetermined signal wavelength and an associated predetermined level of chromatic dispersion; multiplexing said optical signals using a wavelength division multiplexer to<br><br> V' . 16<br><br> 0<br><br> 24 8 1 2 2<br><br> produce a single multiplexed optical signal;<br><br> compensating the chromatic dispersion of said multiplexed optical signal by a predetermined amount so that each of said optical signals within said multiplexed optical signal has a residual optical dispersion; and 5 compensating individually the chromatic dispersion of each of said optical signals to remove therefrom said residual optical dispersion.<br><br>
6. A system for compensating optical dispersion of a plurality of optical signals, comprising:<br><br> a plurality of optical signal transmitters for transmitting a plurality of optical 10 signals;<br><br> a wavelength division multiplexer for generating a multiplexed optical signal from said plurality of optical signals;<br><br> a first dispersion compensating means for compensating the chromatic dispersion of said multiplexed optical signal by a predetermined amount so that each 15 of said optical signals has a residual optical dispersion; and a plurality of second dispersion compensating means for compensating individually the chromatic dispersion of each of said optical signals to remove therefrom said residual optical dispersion.<br><br>
7. A system to increase the usable wavelength range of an optical fibre path, 20 comprising:<br><br> a plurality of optical transmitters for transmitting a plurality of optical signals; wavelength division multiplexing means for multiplexing said optical signals to form a multiplexed optical signal;<br><br> compensating means for the chromatic dispersion of said multiplexed optical j.<br><br> 1 5-<br><br> 24 8 1 2<br><br> signal by a predetermined amount so that each of said optical signals associated with said multiplexed optical signal has a residual optical dispersion; and residual compensating means for compensating individually the chromatic dispersion of each of said optical signals to remove therefrom said residual optical 5 dispersion.<br><br>
8. A system for individually compensating a plurality of optical signal paths prior to multiplexing said optical signals, comprising:<br><br> optical signal transmitting means for transmitting a plurality of optical signals; individual compensating means for compensating individually the chromatic 10 dispersion of each of said optical signals to remove therefrom a predetermined amount of optical chromatic dispersion;<br><br> a wavelength division multiplexer for producing a multiplexed optical signal from said plurality of optical signals; and multiplexed signal compensating means for compensating the chromatic dispersion 15 of said multiplexed optical signal by a predetermined amount so that each of said optical signals has a near zero optical dispersion as a result of combining compensation from said multiplexed signal compensating means and said individual compensating means.<br><br>
9. An optical chromatic dispersion system for simultaneously and independently 20 compensating a plurality of optical signals associated with a wavelength division multiplexer, comprising:<br><br> a plurality of optical signal transmitters for transmitting optical signals each having predetermine frequency;<br><br> wavelength division multiplexer means for multiplexing a predetermined 25 aspect of said optical signals to generate a multiplexed optical signal;<br><br> compensating means for compensating the chromatic dispersion of a<br><br> 18<br><br> 24 8 1 22<br><br> multiplexed optical signal by a predetermined amount so that each of said optical signals has a residual optical dispersion; and compensating means for compensating individually the chromatic dispersion of each of said optical signals to remove therefrom said residual optical dispersion.<br><br> 5
10. A system for matching dispersion compensation to an optical wavelength for a plurality of optical signals that form a multiplexed optical signal, comprising:<br><br> a plurality of optical signal transmitters for transmitting said plurality of optical signals, each of said plurality of optical signals having a predetermined residual chromatic dispersion;<br><br> 10 wavelength division multiplexing means for multiplexing a predetermined aspect of said optical signals to generate a multiplexed optical signal;<br><br> compensating means for compensating the chromatic dispersion of said multiplexed optical signal by a predetermined amount to form said residual optical dispersion for each of said optical signals; and 15 matching compensating means for compensating individually the chromatic dispersion of each of said optical signals to remove therefrom said residual optical dispersion.<br><br>
11. A method for compensating optical chromatic dispersion of a plurality of optical signals substantially as herein described with reference to Figs. 1 to 3 of the 20 accompanying drawings.<br><br> ALCATEL AUSTRALIA LIMITED P.M. Conrick<br><br> 25 Authorized Agent P5/1/1703<br><br> 19<br><br> /,<br><br> </p> </div>
Applications Claiming Priority (1)
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US07/919,426 US5224183A (en) | 1992-07-23 | 1992-07-23 | Multiple wavelength division multiplexing signal compensation system and method using same |
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NZ248122A true NZ248122A (en) | 1996-03-26 |
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FR2681202B1 (en) * | 1991-09-06 | 1993-11-12 | Alcatel Cit | OPTICAL COMMUNICATION LINK WITH CORRECTION OF NON-LINEAR EFFECTS, AND METHOD FOR PROCESSING AN OPTICAL SIGNAL. |
FR2685835A1 (en) * | 1991-12-31 | 1993-07-02 | France Telecom | VERY LONG DISTANCE TRANSMISSION SYSTEM ON OPTICAL FIBER COMPENSATED FOR DISTORTIONS AT RECEPTION. |
FR2685834B1 (en) * | 1991-12-31 | 1995-03-31 | France Telecom | LONG DISTANCE DIGITAL TRANSMISSION SYSTEM ON OPTICAL FIBER WITH DISTORTION COMPENSATION. |
AU664449B2 (en) * | 1992-06-22 | 1995-11-16 | Nec Corporation | Optical communication transmission system |
JP3155837B2 (en) * | 1992-09-14 | 2001-04-16 | 株式会社東芝 | Optical transmission equipment |
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- 1993-07-14 AU AU41903/93A patent/AU667545B2/en not_active Ceased
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AU667545B2 (en) | 1996-03-28 |
US5224183A (en) | 1993-06-29 |
AU4190393A (en) | 1994-01-27 |
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